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JPH0374873B2 - - Google Patents
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JPH0374873B2 - - Google Patents

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Publication number
JPH0374873B2
JPH0374873B2 JP59108620A JP10862084A JPH0374873B2 JP H0374873 B2 JPH0374873 B2 JP H0374873B2 JP 59108620 A JP59108620 A JP 59108620A JP 10862084 A JP10862084 A JP 10862084A JP H0374873 B2 JPH0374873 B2 JP H0374873B2
Authority
JP
Japan
Prior art keywords
wave
component
interference
carrier
phase
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP59108620A
Other languages
Japanese (ja)
Other versions
JPS60253325A (en
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed filed Critical
Priority to JP59108620A priority Critical patent/JPS60253325A/en
Publication of JPS60253325A publication Critical patent/JPS60253325A/en
Publication of JPH0374873B2 publication Critical patent/JPH0374873B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B1/00Details of transmission systems, not covered by a single one of groups H04B3/00 - H04B13/00; Details of transmission systems not characterised by the medium used for transmission
    • H04B1/06Receivers
    • H04B1/10Means associated with receiver for limiting or suppressing noise or interference
    • H04B1/12Neutralising, balancing, or compensation arrangements

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Signal Processing (AREA)
  • Picture Signal Circuits (AREA)
  • Noise Elimination (AREA)

Description

【発明の詳細な説明】 (技術分野) 本発明は、混入した妨害波を除去して残留側波
帯変調方式テレビジヨン放送波などを受信する妨
害波除去受信装置に関し、特に、通常のテレビジ
ヨン受信機に容易に付加し得る程度に簡単な構成
により、受像画質の劣化を伴うことなく、複数の
妨害波を除去し得るようにしたものである。
DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention relates to an interference wave removal receiving device that removes mixed interference waves and receives residual sideband modulation television broadcast waves, and in particular, With a configuration that is simple enough to be easily added to a receiver, a plurality of interference waves can be removed without deteriorating the received image quality.

(従来技術) 従来、受信した残留側波帯変調方式テレビジヨ
ン放送波に混入している妨害波を除去するには、
帯域幅の狭い帯域除去フイルタ、すなわち、いわ
ゆるノツチフイルタを受信機の中間周波数に挿入
してなるべく混入妨害波成分のみを除去するよう
にしていた。しかしながら、かかる従来の妨害波
除去手段によつては、妨害波の周波数が映像搬送
波周波数に近接している場合、特に、残留側波帯
変調方式テレビジヨン放送波の両側波帯伝送帯域
内に妨害波が混入している場合には、ノツチフイ
ルタの挿入により、妨害波を除去してその結果目
障りな妨害波と映像搬送波とのビート成分は一応
除去されても、ノツチフイルタにより妨害波周波
数近傍の映像信号成分も同時に失われるので、受
像画質の十分な改善が困難である、という欠点が
あつた。
(Prior art) Conventionally, in order to remove interference waves mixed in received residual sideband modulation television broadcast waves,
A band rejection filter with a narrow bandwidth, ie, a so-called notch filter, is inserted into the intermediate frequency of the receiver in order to remove only the mixed interference wave component as much as possible. However, with such conventional interference wave removal means, when the frequency of the interference wave is close to the video carrier frequency, especially when the frequency of the interference wave is close to the video carrier frequency, If the interference waves are mixed in, the interfering waves can be removed by inserting a notch filter, and even if the beat component between the disturbing interference waves and the video carrier wave has been removed, the notch filter will remove the video signal near the interfering wave frequency. Since components are also lost at the same time, there is a drawback that it is difficult to sufficiently improve the quality of the received image.

また、別な方法として近接して配設した2本以
上の受信アンテナからの受信波を、振幅および位
相を相対的に調整して合成することによつて形成
した受信アンテナ全体としての指向性のヌル方向
を妨害波到来方向に一致させて妨害波を除去する
ことも従来行なわれていたが、妨害波が電離層ス
ポラデイツクスE層を介しての反射波である場合
のように、伝搬条件の変化により妨害波の到来方
向が変化すれば、その都度ヌル方向の再調整を行
なわなければならず、特に、複数の妨害波を除去
することは極めて困難であるという欠点があつ
た。
Another method is to synthesize the received waves from two or more receiving antennas placed close to each other by relatively adjusting the amplitude and phase. Conventionally, interference waves were removed by aligning the null direction with the arrival direction of the interference wave, but if the interference wave is a reflected wave via the ionospheric sporadic E layer, depending on the propagation conditions, If the arrival direction of the interference waves changes due to a change, the null direction must be readjusted each time, and in particular, there is a drawback that it is extremely difficult to eliminate a plurality of interference waves.

(目的) 本発明の目的は、上述した従来の欠点を除去
し、受信した残留側波帯変調方式テレビジヨン放
送波などの両側波帯伝送帯域に混入して著しい受
信障害を生ずる妨害波を、複数の妨害波が混入し
ている場合であつても、比較的簡単な回路構成に
より、本来の受像画質を損うことなく、安定確実
に除去し得るようにした妨害除去受信装置を提供
することにある。
(Objective) The object of the present invention is to eliminate the above-mentioned conventional drawbacks, and eliminate interference waves that mix into the double-sideband transmission band of received vestigial sideband modulation type television broadcast waves and cause significant reception interference. To provide an interference removal receiving device capable of stably and reliably removing even when a plurality of interference waves are mixed in, without impairing original received image quality, with a relatively simple circuit configuration. It is in.

本発明の他の目的は、テレビジヨン中継放送用
受信設備や家庭用受像機など従来慣用のテレビジ
ヨン受信装置における中間周波段に本発明による
簡単な構成の回路を付加することにより上述した
種類の混入妨害波を容易に除去し得るようにした
妨害波除去受信装置を提供することにある。
Another object of the present invention is to provide the above-mentioned type of circuit by adding a circuit having a simple configuration according to the present invention to an intermediate frequency stage of a conventional television receiver such as a television relay broadcast receiving equipment or a home receiver. It is an object of the present invention to provide an interference wave removal receiving device that can easily remove mixed interference waves.

(発明の要点) すなわち、本発明妨害波除去受信装置は、残留
側波帯変調方式テレビジヨン放送波など変調波の
搬送信号成分の復調信号の直角位相成分として
は、両側波帯伝送される信号成分は現われず、単
側波帯伝送される信号成分のみとなり、その中に
は妨害波も現われる、ということを巧みに利用し
て抽出した妨害波により、受信変調波の搬送信号
成分に混入している妨害波を相殺して、混入妨害
波のみを十分に除去し得るようにしたものであ
り、妨害波を含めて受信した両側波帯伝送成分を
有する変調波の搬送信号成分から搬送波成分を再
生する搬送再生手段と、その手段により再生した
前記搬送波成分をπ/2移相する搬送波移相手段
と、その手段によりπ/2移相した前記再生搬送波
成分により両側波帯伝送帯域の前記受信した変調
波の搬送信号成分を同期検波して直角位相成分を
抽出する同期検波手段と、前記直角位相成分によ
り前記再生してπ/2移相した搬送波成分を変調す
る変調手段と、その手段の出力を波して前記受
信した変調波の搬送信号成分から識別した前記妨
害波と同一の周波数成分を抽出する少なくとも1
個の波手段と、前記受信した変調波の搬送信号
成分から前記抽出した同一の周波数成分を減算し
て前記両側波帯伝送成分中に混入した前記妨害波
を相殺除去する減算手段とを備えたことを特徴と
するものである。
(Summary of the Invention) In other words, the interference wave removal receiving device of the present invention uses a signal transmitted in both sidebands as a quadrature phase component of a demodulated signal of a carrier signal component of a modulated wave such as a vestigial sideband modulation type television broadcast wave. component does not appear, only the signal component that is transmitted in a single sideband, and interference waves also appear among them.The interference wave extracted by skillfully taking advantage of this fact is mixed into the carrier signal component of the received modulated wave. This system is designed to cancel out the interfering interference waves and sufficiently remove only the mixed interference waves. carrier regeneration means for regenerating; carrier phase shifting means for shifting the phase of the carrier wave component regenerated by the means by π/2; synchronous detection means for synchronously detecting a carrier signal component of a modulated wave to extract a quadrature phase component; a modulation means for modulating the reproduced carrier wave component phase-shifted by π/2 by the quadrature phase component; at least one frequency component that is the same as the interference wave identified from the carrier signal component of the received modulated wave by extracting the same frequency component as the interference wave.
and subtraction means for subtracting the extracted same frequency component from the carrier signal component of the received modulated wave to cancel out and remove the interference wave mixed into the double sideband transmission component. It is characterized by this.

(実施例) 以下に図面を参照して実施例につき本発明を詳
細に説明する。
(Example) The present invention will be described in detail below with reference to the drawings.

まず、本発明の理解を容易にするために、残留
側波帯変調方式テレビジヨン放送波について、側
波帯分布特性、同相成分分布特性および直角位相
成分分布特性を第1図a,bおよびcにそれぞれ
示す。すなわち、テレビジヨン放送波の同図aに
示す側波帯分布は、同図bに示す同相成分と同図
cに示す直角位相成分とに分けられる。
First, in order to facilitate understanding of the present invention, the sideband distribution characteristics, in-phase component distribution characteristics, and quadrature component distribution characteristics of vestigial sideband modulation television broadcast waves are shown in FIGS. 1a, b, and c. are shown respectively. That is, the sideband distribution of the television broadcast wave shown in FIG. 2A is divided into an in-phase component shown in FIG.

いま、テレビジヨン放送波における映像信号を
G(t)とし、映像搬送波角周波数をωpとしたと
き、振幅変調テレビジヨン放送波がなす振幅変調
波G(t)cpsωptを第1図aに示すような側波帯
分布特性により残留側波帯伝送した場合に、その
振幅変調波はつぎの(1)式によつて表わされる。
Now, when the video signal in the television broadcast wave is G(t) and the video carrier angular frequency is ω p , the amplitude modulated wave G(t) cps ω p t produced by the amplitude modulated television broadcast wave is shown in Fig. 1. When the vestigial sideband is transmitted using the sideband distribution characteristic as shown in a, the amplitude modulated wave is expressed by the following equation (1).

C(t)cps(ωpt+θp) −S(t)sio(ωpt+θp) (1) ここに、θpは映像搬送波角周波数ωpにおける位
相であり、また、C(t)およびS(t)は、それ
ぞれ、第1図bおよびcに示す同相成分および直
角位相成分の各分布特性について映像搬送波角周
波数ωpを0にシフトしたときの伝達関数をそれ
ぞれ有する回路に映像信号G(t)を加えたとき
にそれぞれ得られる出力応答である。
C(t) cpsp t+θ p ) −S(t) siop t+θ p ) (1) Here, θ p is the phase at the image carrier angular frequency ω p , and C(t) and S(t) is a video signal G applied to a circuit having a transfer function when the video carrier angular frequency ω p is shifted to 0 for each distribution characteristic of the in-phase component and the quadrature component shown in FIGS. 1b and 1c, respectively. These are the output responses obtained when adding (t).

しかして、(1)式によつて表わされる振幅変調波
をつぎの(2)式によつて表わされる相対位相の搬送
波によつて同期検波すると、同相成分C(t)が
得られる。
Therefore, when the amplitude modulated wave expressed by equation (1) is synchronously detected using a carrier wave having a relative phase expressed by the following equation (2), an in-phase component C(t) is obtained.

cos(ωpt+θp) (2) 一方、この(2)式によつて表わされる搬送波を
π/2遅らせて得られる同搬送波とは位相がπ/2だ
け異なるつぎの(3)式によつて表わされる相対位相
の搬送波によつて(1)式の振幅変調波を同期検波す
ると、直角位相成分S(t)が得られる。
cos (ω p t + θ p ) (2) On the other hand, the carrier wave expressed by this equation (2) is obtained by delaying the carrier wave by π/2, and the phase is different by π/2 according to the following equation (3). When the amplitude modulated wave of equation (1) is synchronously detected using a carrier wave with a relative phase expressed as , a quadrature phase component S(t) is obtained.

sin(ωpt+θp) (3) この場合、前述したように残留側波帯変調方式
のテレビジヨン放送波が両側波帯伝送される0〜
μの角周波数領域には映像信号成分を含まない直
角位相成分S(t)のみが得られる。しかして、
第1図a〜cに示すように、上述の角周波数領域
0〜μに相当する両側波帯伝送帯域内に、つぎの
(4)式によつて表わされる角周波数ωp+δの妨害
波が混入したとする。
sin (ω p t + θ p ) (3) In this case, as mentioned above, the vestigial sideband modulation method television broadcast wave is transmitted in both sidebands.
In the angular frequency region of μ, only the quadrature phase component S(t), which does not include the video signal component, is obtained. However,
As shown in Figures 1a to 1c, within the double sideband transmission band corresponding to the angular frequency range 0 to μ mentioned above, the following
Suppose that an interference wave with an angular frequency ω p +δ expressed by equation (4) is mixed.

Acos{(ωp+δ)t+(θp+φ〓)} (4) ここに、(θp+φ〓)は妨害波の相対位相であり、
Aはその振幅の絶対値である。
Acos {(ω p + δ)t + (θ p +φ〓)} (4) Here, (θ p +φ〓) is the relative phase of the disturbance wave,
A is the absolute value of its amplitude.

この(4)式の妨害波を、上述のように振幅変調波
をそれぞれ同期検波したのと同一の(2)式および(3)
式によつてそれぞれ表わされる搬送波によつて同
様に同期検波すると、つぎの(5)式によつて表わさ
れる同相成分およびつぎの(6)式によつて表わされ
る直角位相成分が同期検波出力としてそれぞれ得
られる。
This interference wave in equation (4) can be detected using equations (2) and (3), which are the same as those obtained by synchronously detecting the amplitude modulated waves as described above.
When similarly synchronously detecting the carrier waves expressed by the following equations, the in-phase component expressed by the following equation (5) and the quadrature phase component expressed by the following equation (6) are obtained as the synchronous detection output. You can get each.

A/2cos(δt+φ〓)+1/2C(t) (5) −A/2sin(δt+φ〓)−1/2S(t)(6
) かかる妨害波の同期検波出力のうち、(6)式の直
角位相成分を帯域値μを有するバンドパスフイル
タもしくはローパスフイルタに導いて上述した(6)
式の第1項の成分、すわなち、つぎの(7)式によつ
て表わされる妨害波直角位相成分を取出す。
A/2cos(δt+φ〓)+1/2C(t) (5) −A/2sin(δt+φ〓)−1/2S(t)(6
) Out of the synchronous detection output of such interference waves, the quadrature component of equation (6) is guided to a bandpass filter or low-pass filter having a band value μ, and the above-mentioned (6)
The component of the first term of the equation, that is, the quadrature phase component of the interference wave expressed by the following equation (7) is extracted.

−A/2sin(δt+φ〓) (7) この(7)式の妨害波直角位相成分を(3)式の直角位
相搬送波と乗算すると、つぎの(8)式によつて表わ
される妨害波直角位相成分のよる振幅変調波が得
られる。
−A/2sin(δt+φ〓) (7) Multiplying the quadrature phase component of the disturbance wave in equation (7) by the quadrature phase carrier wave in equation (3), the quadrature phase of the disturbance wave expressed by the following equation (8) is obtained. An amplitude modulated wave with different components is obtained.

A/4cos{(ωp+δ)t+(θp+φ〓)} A/4cos{(ωp−δ)t+(θp−φ〓)}(8) この(8)式の第1項によつて表わされる角周波数
ωp+δの妨害波成分をバンドパスフイルタもし
くはハイパスフイルタによつて分離抽出し、その
振幅を4倍すると、(4)式によつて表わした混入妨
害波と全く同一の妨害波成分が得られることにな
る。
A/4cos {(ω p +δ)t+(θ p +φ〓)} A/4cos{(ω p −δ)t+(θ p −φ〓)}(8) According to the first term of this equation (8), If we separate and extract the interference wave component with the angular frequency ω p +δ expressed by using a bandpass filter or high-pass filter and multiply its amplitude by 4, we can obtain exactly the same interference as the mixed interference wave expressed by equation (4). The wave component will be obtained.

したがつて、両側波帯伝送帯域内に混入してい
る(4)式の妨害波は、(8)式の第1項による妨害波成
分を逆位相加算することによつて相殺除去するこ
とができ、その際映像信号成分には何らの変化も
及ぼさず、その結果、混入妨害波のみをほぼ完全
に除去した本来の振幅変調テレビジヨン放送波が
得られる。
Therefore, the interference wave of equation (4) mixed in the double-sideband transmission band can be canceled out and removed by adding the interference wave component of the first term of equation (8) in antiphase. At this time, the video signal component is not changed in any way, and as a result, the original amplitude modulated television broadcast wave from which only the interfering interference waves are almost completely removed is obtained.

以上においては、妨害波が振幅変調テレビジヨ
ン放送波の両側波帯伝送帯域中の、特に上側波帯
の部分に混入したものとし(4)式によつて表わされ
る妨害波を仮定したが、妨害波が両側波帯伝送帯
域中の下側波帯の部分に混入した場合には以下の
ようにする。
In the above, it is assumed that the interference wave is mixed in the upper sideband part of the both sideband transmission band of the amplitude modulated television broadcast wave, and that the interference wave is expressed by equation (4). When a wave enters the lower sideband portion of the doublesideband transmission band, the following procedure is performed.

すなわち、この場合の妨害波を(9)式によつて表
わす。
That is, the interference wave in this case is expressed by equation (9).

Bcos{(ωp−δ)t+(θp+φ〓)} (9) ここに(θp+φ〓)は妨害波の相対位相であり、
Bはその振幅の絶対値である。
Bcos {(ω p −δ)t+(θ p +φ〓)} (9) Here, (θ p +φ〓) is the relative phase of the interference wave,
B is the absolute value of its amplitude.

この(9)式の妨害波を(3)式によつて表わされる搬
送波によつて同期検波すると、つぎの(10)式によつ
て表わされる直角位相成分が同期検波出力として
得られる。
When the interference wave expressed by equation (9) is synchronously detected using the carrier wave expressed by equation (3), a quadrature phase component expressed by the following equation (10) is obtained as a synchronous detection output.

B/2sin(δt−φ〓)−1/2S(t)(10) この直角位相成分を帯域幅μを有するバンドパ
スフイルタもしくはローパスフイルタに導いて(10)
式の第1項の成分、すなわち、つぎの(11)式に
よつて表わされる妨害波直角位相成分を取出す。
B/2sin(δt−φ〓)−1/2S(t)(10) This quadrature component is guided to a bandpass filter or lowpass filter with a bandwidth μ(10)
The component of the first term of the equation, that is, the interference wave quadrature component expressed by the following equation (11) is extracted.

B/2sin(δt−φ〓) (11) この(11)式の妨害直角位相成分を(3)式の直角
位相搬送波と乗算すると、つぎの(12)式によつ
て表わされる妨害波直角位相成分による振幅変調
波が得られる。
B/2sin(δt−φ〓) (11) Multiplying the quadrature phase component of the disturbance in equation (11) by the quadrature carrier in equation (3), the quadrature phase of the disturbance wave expressed by the following equation (12) is obtained. An amplitude modulated wave by the component is obtained.

B/4cos{(ωp−δ)t+(θp+φ〓)} −B/4cos{(ωp+δ)t+(θp−φ〓)}
(12) この(12)式の第1項によつて表わされる角周
波数ωp−δの妨害波成分をバンドパスフイルタ
もしくはローパスフイルタによつて分離抽出し、
その振幅を4倍とすると(9)式によつて表わした混
入妨害波と全く同一の妨害波成分が得られること
になり、上側波帯に妨害波が混入した場合とまつ
たく同様にして妨害波成分の相殺除去を行うこと
ができる。
B/4cos {(ω p −δ)t+(θ p +φ〓)} −B/4cos{(ω p +δ)t+(θ p −φ〓)}
(12) Separate and extract the interference wave component of the angular frequency ω p −δ expressed by the first term of equation (12) using a band pass filter or a low pass filter,
If the amplitude is quadrupled, a disturbance wave component that is exactly the same as the mixed interference wave expressed by equation (9) will be obtained, and the interference will occur in exactly the same way as when the interference wave mixes in the upper sideband. It is possible to cancel and remove wave components.

上述のような動作原理によつて混入妨害波を相
殺除去する本発明妨害波除去受信装置の基本的構
造の例を第2図に示す。図示の構成例において
は、妨害波が前述したような態様にて混入した残
留側波帯変調方式テレビジヨン放送波を受信し、
周波数変換して得た中間周波(IF)信号を入力
端子から搬送波再生回路1に導いて、その搬送信
号成分からの映像搬送波と同相の搬送波成分を再
生し、その再生搬送波成分をπ/2移相遅れ回路2
に導いて上述の映像搬送波に対して直角位相を有
する搬送波成分を形成する。ついで、その直角位
相搬送波成分を乗算器8に供給し、入力端子から
導いたIF信号に乗算して同期検波を施し、かか
る直角位相同期検波出力を、テレビジヨン放送波
の両側波帯伝送帯域相当の通過帯域を有するロー
パスフイルタ4を介して乗算器5に導き、他方で
は直角位相同期検波出力のローパスフイルタ4に
おける位相遅延に対応して位相を補償するための
位相補償回路6を介してπ/2移相遅れ回路2から
の直角位相搬送成分をも乗算器5に供給し、これ
ら相互間で乗算を行なつて振幅変調を施し、(8)式
乃至(12)式の妨害波直角位相成分による振幅変
調波を正確に再現する。かかる乗算器5からの乗
算出力をバンドパスフイルタ7および8に導い
て、両側波帯伝送帯域中の上側波帯成分および下
側波帯成分をそれぞれ波抽出し得るようにす
る。かかるバンドパスフイルタ7および8の波
出力を切換器12に導き、後述するようにして妨
害波が上下各側波帯のいずれに混入しているかを
識別した結果に応じ、いずれか一方の波出力を
切換えて取出し、レベル調整回路9によりレベル
を調整したうえで減算回路11に導き、以上の信
号処理による遅れ時間を補償するための遅延回路
10を介して入力端子から供給したIF信号から
減算すれば、IF信号から混入妨害波のみを相殺
除去した本来のIF信号が出力端子から取出され
る。
FIG. 2 shows an example of the basic structure of the interference wave cancellation receiving apparatus of the present invention which cancels and eliminates mixed interference waves based on the above-mentioned operating principle. In the illustrated configuration example, a vestigial sideband modulation type television broadcast wave mixed with interference waves in the manner described above is received,
The intermediate frequency (IF) signal obtained by frequency conversion is guided from the input terminal to the carrier wave regeneration circuit 1, a carrier wave component in phase with the video carrier wave from the carrier signal component is regenerated, and the regenerated carrier wave component is shifted by π/2. Phase delay circuit 2
to form a carrier wave component having a phase quadrature with respect to the image carrier wave described above. Next, the quadrature phase carrier wave component is supplied to the multiplier 8, where it is multiplied by the IF signal led from the input terminal and subjected to synchronous detection. π/ The quadrature phase carrier component from the two-phase shift/delay circuit 2 is also supplied to the multiplier 5, and these components are multiplied together to perform amplitude modulation, thereby generating the quadrature phase component of the interference wave from equations (8) to (12). Accurately reproduces amplitude modulated waves. The multiplication output from the multiplier 5 is guided to bandpass filters 7 and 8 so that upper and lower sideband components in the double-sideband transmission band can be extracted, respectively. The wave outputs of the bandpass filters 7 and 8 are guided to the switching device 12, and depending on the result of identifying which of the upper and lower sidebands the interference wave is mixed in as will be described later, the wave output of either one is changed. After adjusting the level using the level adjustment circuit 9, the signal is sent to the subtraction circuit 11, and is subtracted from the IF signal supplied from the input terminal via the delay circuit 10 to compensate for the delay time caused by the above signal processing. For example, the original IF signal obtained by canceling and removing only the mixed interference waves from the IF signal is taken out from the output terminal.

したがつて、第2図示の構成による本発明妨害
波除去受信装置においては、テレビジヨン放送波
の両側波帯伝送帯域中、上下いずれの側波帯に混
入している妨害波も、その妨害波の混入帯域を識
別した結果に応じ、上下各側波帯をそれぞれ通過
帯域とする2個のバンドパスフイルタ7および8
を選択的に使用することにより、確実容易に除去
することができる。また、混入妨害波の数も、1
波でなく、複数波であつてもよい。
Therefore, in the interference wave removal receiver of the present invention having the configuration shown in FIG. According to the result of identifying the mixed band of
By selectively using , you can ensure easy removal. Also, the number of mixed interference waves is 1
It may be multiple waves instead of one wave.

以上の説明においては、テレビジヨン放送波の
両側波帯伝送帯域中、上下いずれかの側波帯に単
一乃至複数の妨害波が混入している場合における
本発明妨害波除去受信装置の構成例について述べ
たが、上下両側波帯に同時にそれぞれ単一乃至複
数の妨害波が混入している場合に、それら上下両
側波帯の妨害波を上述したと同様にして相殺除去
するようにした本発明受信装置の構成例を第3図
に示す。
In the above explanation, an example of the configuration of the interference wave removal receiving device of the present invention is used when single or multiple interference waves are mixed in either the upper or lower sideband of the double-sideband transmission band of the television broadcast wave. However, in the case where single or multiple interference waves are mixed simultaneously in both the upper and lower sidebands, the present invention is designed to cancel and remove the interference waves in the upper and lower sidebands in the same manner as described above. An example of the configuration of the receiving device is shown in FIG.

いま、テレビジヨン放送波の上側波帯および下
側波帯にそれぞれ混入した妨害波をつぎの(13)
式および(14)式によつて表わすものとする。
Now, the interference waves mixed in the upper and lower sidebands of the television broadcast waves are expressed as follows (13).
and (14).

Acos{(ωp+δu)t+(θp+φ〓u)} (13) Bcos{(ωp−δl)t+(θp+φ〓l)} (14) しかして、第3図示の構成例は、第2図示の構
成例と比較すれば明らかなように、第2図示の構
成例においてバンドパスフイルタ7および8と切
換器12とにより乗算器5の乗算出力のうち、上
側波帯成分と下側波帯成分とを選択的に切換えて
取出す回路部分を、両側波帯伝送帯域を分割した
複数の周波数帯域をそれぞれ通過帯域とするn個
のバンドパスフイルタ13−1〜13−nとそれ
らのフイルタ13−1〜13−nの波出力を開
閉して選択的に取出し得るようにしたn個の開閉
スイツチSW1〜SWoに置換して、要すれば最大n
個の混入妨害波をそれぞれ相対除去し得るように
したものである。
Acos {(ω p + δ u )t+(θ p +φ〓 u )} (13) Bcos {(ω p −δ l )t+(θ p +φ〓 l )} (14) Therefore, the configuration example shown in the third figure As is clear from a comparison with the configuration example shown in the second figure, in the configuration example shown in the second figure, the bandpass filters 7 and 8 and the switch 12 separate the upper sideband component from the multiplication output of the multiplier 5. The circuit portion for selectively switching and extracting the lower sideband components includes n bandpass filters 13-1 to 13-n each having a pass band corresponding to a plurality of frequency bands obtained by dividing the doublesideband transmission band. The wave outputs of the filters 13-1 to 13-n are replaced with n open/close switches SW 1 to SW o that can be selectively taken out by opening and closing the wave outputs, and if necessary, the wave outputs of the filters 13-1 to 13-n can be selectively extracted.
It is possible to relatively eliminate each of the mixed interference waves.

しかして、(13)式および(14)式によつて表
わされる妨害波が同時に混入したIF信号を、(3)
式によつて表わされる直角位相搬送波を乗算器3
に供給して同期検波すると、ローパスフイルタ4
の出力につぎの(15)式によつて表わされる妨害
波の直角位相成分が得られる。
Therefore, the IF signal mixed with the interference waves expressed by equations (13) and (14) at the same time can be expressed as (3)
The quadrature carrier wave multiplier 3 is expressed by
When synchronously detected by supplying to
The quadrature phase component of the interference wave expressed by the following equation (15) is obtained at the output of .

−A/2sin(δut+φ〓u) +B/2sin(δlt−φ〓l) (15) つぎにこの(15)式によつて表わされるローパ
スフイルタ4の出力と(3)式によつて表わされる直
角位相搬送波との掛算を行なう乗算器5の出力Ei
は、(13)式および(14)式による上側波帯およ
び下側波帯の混入妨害波に対して、つぎの(16)
式によつて表わすことができる。
−A/2sin(δ u t+φ〓 u ) +B/2sin(δ l t−φ〓 l ) (15) Next, the output of the low-pass filter 4 expressed by this equation (15) and the output of the low-pass filter 4 expressed by equation (3) are The output E i of the multiplier 5 performs multiplication with the quadrature carrier wave represented by
For mixed disturbance waves in the upper sideband and lower sideband according to equations (13) and (14), the following equation (16) is obtained.
It can be expressed by the formula.

Ei=−A/2sin(δut+φ〓u)・sin(ωpt+θp
+B/2sin(δlt−φ〓l)・sin(ωpt+θp) =A/4cos{(ωp+δu)t+(θp+φ〓u)}
−A/4cos{(ωp−δu)t+(θp−φ〓u)} −B/4cos{(ωp+δl)t+(θp−φ〓l
}+B/4cos{(ωp−δl)t+(θp+φ〓l)}(1
6) この(16)式の最右辺における第1項、第2
項、第3項および第4項をそれぞれAu,Al,Bu
Blと表わすと、これら各成分のスペクトル分布は
第4図に示すようになる。
E i =-A/2sin(δ u t+φ〓 u )・sin(ω p t+θ p
+B/2sin(δ l t−φ〓 l )・sin(ω p t+θ p ) =A/4cos {(ω pu )t+(θ p +φ〓 u )}
−A/4cos {(ω p −δ u )t+(θ p −φ〓 u )} −B/4cos {(ω pl )t+(θ p −φ〓 l )
}+B/4 cos {(ω p −δ l )t+(θ p +φ〓 l )}(1
6) The first and second terms on the right-most side of equation (16)
term, the third term, and the fourth term respectively as A u , A l , B u ,
When expressed as B l , the spectral distribution of each of these components is as shown in FIG.

しかして、第3図示の構成例における遅延回路
10の遅延出力IF信号に含まれる妨害波成分は
第4図示のスペクトル分布において上下各側波帯
領域にそれぞれ現われる各成分AuとBlとである
から、これらの各スペクトル成分をバンドパスフ
イルタ13−1〜13−nを用いてそれぞれ抽出
し、さらに開閉スイツチSW1〜SWoにより選択的
に取出せば、減算回路11における相殺除去によ
り、遅延出力IF信号に同時に混入している複数
の妨害波を、第2図示の構成例におけると同様に
して、一挙に相殺除去することができる。したが
つて、本発明受信装置における振幅変調を行なう
乗算器の出力を各妨害波の帯域とほぼ同一の通過
帯域をそれぞれ有して中心周波数が順次に異なる
複数個のバンドパスフイルタに導いて上下それぞ
れの側波帯に混入している単一乃至複数の混入妨
害波を一斉にそれぞれ相殺除去することができ
る。
Therefore, the interference wave components included in the delayed output IF signal of the delay circuit 10 in the configuration example shown in FIG . Therefore, if each of these spectral components is extracted using the bandpass filters 13-1 to 13-n and then selectively extracted by the on/off switches SW1 to SW0 , the delay is reduced by canceling the subtraction circuit 11. A plurality of interference waves mixed into the output IF signal at the same time can be canceled out and removed at once in the same manner as in the configuration example shown in the second figure. Therefore, in the receiver of the present invention, the output of the multiplier that performs amplitude modulation is guided to a plurality of bandpass filters each having a pass band that is almost the same as the band of each interference wave and whose center frequency is different sequentially. Single or multiple mixed interference waves mixed in each sideband can be canceled out and removed at the same time.

なお、上記において使用するバンドパスフイル
タとしては、妨害波がスポラデイツクスE層を介
しての外国のFM放送波である場合、FM放送波
の配置は100KHzおきであるから、中心周波数を
100KHz間隔とした通常のFM放送波受信機に使用
されてるものと同等の特性を有するバンドパスフ
イルタを用いるのが好ましい。
In addition, as for the bandpass filter used in the above, if the interfering wave is a foreign FM broadcast wave via Sporadics E layer, the FM broadcast waves are arranged every 100KHz, so the center frequency should be set to
It is preferable to use a bandpass filter having characteristics similar to those used in a normal FM broadcast wave receiver with an interval of 100KHz.

第3図示の構成における開閉スイツチSW1
SWoは、混入妨害波の個数および周波数に応じ、
バンドパスフイルタ13−1〜13−nのうちい
ずれのフイルタの波出力を用いるかを選択する
ものであり、かかる開閉スイツチSW1〜SWoの制
御は、例えば第5図に示す構成の切換信号発生装
置を用いて自動的に行なうことができる。図示の
構成による切換信号発生装置においては、例え
ば、スポラデイツクE層による外国FM電波の混
信のように、妨害波が角度変調波である場合に、
テレビジヨン放送波は振幅変調波であることを利
用して、局部発振周波数を掃引しながら入力IF
信号を周波数変換することによりスペクトルアナ
ライザのようにそのIF信号帯域内の各周波数成
分を順次に一定周波数に変換して角度変調波を復
調し、混入妨害角度変調波成分を順次に検出して
それぞれの周波数と混入個数とを識別し、その識
別結果を切換信号として取出し、その切換信号に
基づいて開閉スイツチの制御を行なう。
Opening/closing switch SW 1 in the configuration shown in the third diagram
SW o depends on the number and frequency of mixed interference waves,
The wave output of one of the bandpass filters 13-1 to 13-n is selected to be used, and the on/off switches SW 1 to SW o are controlled by a switching signal having the configuration shown in FIG. 5, for example. This can be done automatically using a generator. In the switching signal generator having the configuration shown in the figure, when the interference wave is an angle modulated wave, such as interference of foreign FM radio waves by the Sporadic E layer, for example,
Taking advantage of the fact that television broadcast waves are amplitude modulated waves, the input IF is adjusted while sweeping the local oscillation frequency.
By converting the frequency of the signal, each frequency component within the IF signal band is sequentially converted to a constant frequency like a spectrum analyzer to demodulate the angle modulated wave, and the interfering interference angle modulated wave components are sequentially detected and each The frequency and number of mixed particles are identified, the identification result is taken out as a switching signal, and the open/close switch is controlled based on the switching signal.

すなわち、入力IF信号を乗算器16に導き、
電圧制御発振器15から供給する掃引局部発振出
力を乗算して周波数変換を施し、その変換出力を
狭帯域のバンドパスフイルタ17、リミツタ18
を介してFM検波回路19に供給して角度変調波
を復調し、その検波出力を整流回路20により直
流電圧に変換する。したがつて、整流回路20か
らは混入した妨害角度変調波を検出する都度、出
力直流電圧が得られる。その出力直流電圧をA−
Dコンバータ21によりデイジタルデータに変換
して演算処理装置(CPU)22に導き、混入妨
害波の周波数に対応したバンドパスフイルタ13
−1〜13−nのいずれかの波出力を取出すよ
うに開閉スイツチSW1〜SWoを制御する切換信号
を発生させる。なお、かかる混入妨害波検出の状
態を参照してCPU22からデイジタル掃引信号
を送出し、D−Aコンバータ23を介して電圧制
御発振器15の発振周波数を掃引する。
That is, the input IF signal is guided to the multiplier 16,
Frequency conversion is performed by multiplying the swept local oscillation output supplied from the voltage controlled oscillator 15, and the converted output is passed through a narrowband bandpass filter 17 and a limiter 18.
The angle modulated wave is supplied to the FM detection circuit 19 via the FM detection circuit 19 to demodulate the angle modulated wave, and the detection output is converted into a DC voltage by the rectification circuit 20. Therefore, an output DC voltage is obtained from the rectifier circuit 20 each time the mixed interfering angle modulated wave is detected. Its output DC voltage is A-
The data is converted into digital data by a D converter 21 and sent to a processing unit (CPU) 22, where it is passed through a bandpass filter 13 corresponding to the frequency of the mixed interference wave.
A switching signal is generated to control the on/off switches SW 1 to SW o so as to extract any one of wave outputs from -1 to 13-n. Note that, referring to the state of mixed interference wave detection, the CPU 22 sends out a digital sweep signal to sweep the oscillation frequency of the voltage controlled oscillator 15 via the DA converter 23.

したがつて、図示の構成による切換信号発生装
置は、周波数変換した角度変調の形態の混入妨害
波がバンドパスフイルタ17を通過する都度、整
流回路20から出力直流電圧が得られ、その出力
直流電圧値によつて妨害波の周波数を識別すると
ともに混入個数を知ることができる。
Therefore, in the switching signal generating device having the configuration shown in the figure, an output DC voltage is obtained from the rectifier circuit 20 each time the mixed interference wave in the form of frequency-converted angle modulation passes through the bandpass filter 17, and the output DC voltage is The value allows the frequency of the interference waves to be identified and the number of interfering waves to be determined.

(効果) 以上の説明から明らかなように、本発明によれ
ば、残留側波帯変調方式テレビジヨン放送波の両
側波帯伝送帯域に、上側波帯、下側波帯の別を問
わず、混入している複数の妨害波を同時に相殺除
去することができ、また、受信装置の中間周波段
においてかかる妨害波相殺除去を行なうので、放
送波中継用受信装置や家庭用受像機等の慣用のテ
レビジヨン放送波受信装置に妨害波除去機能を容
易に付加することができ、従来慣用の構成要素を
用いた回路構成のわずかな改修によつてその妨害
波除去機能を達成することができる。なお、この
ような回路構成の簡易さを目的としない場合、あ
るいは特殊な場合、テレビジヨン放送波そのまま
の高周波で行つてよいこと勿論である。
(Effects) As is clear from the above description, according to the present invention, in the double sideband transmission band of the vestigial sideband modulation type television broadcast wave, regardless of whether it is an upper sideband or a lower sideband, Multiple interfering interference waves can be canceled out at the same time, and since such interference waves are canceled out and removed at the intermediate frequency stage of the receiving device, it is possible to cancel out and remove the interference waves at the same time. An interference wave removal function can be easily added to a television broadcast wave receiving device, and the interference wave removal function can be achieved by a slight modification of the circuit configuration using conventional components. It should be noted that, of course, in cases where such simplicity of the circuit configuration is not the objective, or in special cases, the same high frequency as the television broadcast waves may be used.

また、混入妨害波の検出に、映像信号成分が含
まれない両側波帯伝送帯域における直角位相同期
検波出力を用いているので、映像信号成分を損傷
することなく混入妨害波のみを相殺除去して良好
な受像画質を得ることができる。
In addition, since the quadrature phase synchronized detection output in the double-sided transmission band, which does not include the video signal component, is used to detect mixed interference waves, only the mixed interference waves can be canceled out and removed without damaging the video signal component. Good received image quality can be obtained.

したがつて、本発明によれば、混入妨害波の変
調、無変調の別を問わず、また、変調形式の如何
を問わず、さらに、残留側波帯変調方式のテレビ
ジヨン放送波に限らず、両側波帯伝送成分を有す
る変調波に搬送波に対して非対称に混入したあら
ゆる妨害波を、その混入個数や周波数分布の如
何、あるいは、その変化の有無に拘らず、十分に
除去し得る、という格別の効果が得られる。
Therefore, according to the present invention, regardless of whether the mixed interference wave is modulated or not modulated, regardless of the modulation format, and not limited to television broadcast waves using the vestigial sideband modulation method. It is said that it is possible to sufficiently eliminate all interference waves mixed asymmetrically with respect to the carrier wave into a modulated wave having double-sideband transmission components, regardless of the number of interference waves mixed in, the frequency distribution, or whether or not there is a change in the interference waves. A special effect can be obtained.

【図面の簡単な説明】[Brief explanation of drawings]

第1図a,bおよびcは残留側波帯変調方式テ
レビジヨン放送波の側波帯分布特性、同相成分分
布特性および直角位相成分分布特性をそれぞれ示
す特性曲線図、第2図は本発明妨害波除去受信装
置の構成例を示すブロツク線図、第3図は同じく
その受信装置の他の構成例を示すブロツク線図、
第4図は同じくその構成例における回路動作の例
を示すスペクトル分布図、第5図は同じくその構
成例における開閉スイツチ切換信号発生装置の構
成例を示すブロツク線図である。 1……搬送波再生回路、2……π/2移相遅れ回
路、8,5,16……乗算器、4……ローパスフ
イルタ、6……位相補償回路、7,8,13−1
〜13−n,17……バンドパスフイルタ、9…
…レベル調整回路、10……遅延回路、11……
減算回路、12……切換器、15……電圧制御発
振器、18……リミツタ、19……FM検波回
路、20……整流回路、21……A−Dコンバー
タ、22……演算処理装置(CPU)、23……D
−Aコンバータ、SW1〜SWo……開閉スイツチ。
Figures 1a, b, and c are characteristic curve diagrams showing the sideband distribution characteristics, in-phase component distribution characteristics, and quadrature component distribution characteristics of a television broadcast wave using the vestigial sideband modulation method, respectively, and Figure 2 is a characteristic curve diagram showing the present invention interference. FIG. 3 is a block diagram showing an example of the configuration of a wave cancellation receiving device; FIG. 3 is a block diagram showing another example of the configuration of the receiving device;
FIG. 4 is a spectrum distribution diagram showing an example of circuit operation in the same configuration example, and FIG. 5 is a block diagram showing a configuration example of the on-off switch switching signal generating device in the same configuration example. 1... Carrier wave regeneration circuit, 2... π/2 phase shift delay circuit, 8, 5, 16... Multiplier, 4... Low pass filter, 6... Phase compensation circuit, 7, 8, 13-1
~13-n, 17...Band pass filter, 9...
...Level adjustment circuit, 10...Delay circuit, 11...
Subtraction circuit, 12... Switcher, 15... Voltage controlled oscillator, 18... Limiter, 19... FM detection circuit, 20... Rectifier circuit, 21... A-D converter, 22... Arithmetic processing unit (CPU ), 23...D
-A converter, SW 1 ~ SW o ... Open/close switch.

Claims (1)

【特許請求の範囲】 1 妨害波を含めて受信した両側波帯伝送成分を
有する変調波の搬送信号成分から搬送波成分を再
生する搬送波再生手段と、その手段により再生し
た前記搬送波成分をπ/2移相する搬送波移相手段
と、その手段によりπ/2移相した前記再生搬送波
成分により両側波帯伝送帯域の前記受信した変調
波の搬送信号成分を同期検波して直角位相成分を
抽出する同期検波手段と、前記直角位相成分によ
り前記再生してπ/2移相した搬送波成分を変調す
る変調手段と、その手段の出力を波して前記受
信した変調波の搬送信号成分から識別した前記妨
害波と同一の周波数成分を抽出する少なくとも1
個の波手段と、前記受信した変調波の搬送信号
成分から前記抽出した同一の周波数成分を減算し
て前記両側波帯伝送成分中に混入した前記妨害波
を相殺除去する減算手段とを備えたことを特徴と
する妨害波除去受信装置。 2 特許請求の範囲第1項記載の受信装置におい
て、それぞれ異なる波帯域を有する複数個の前
記波手段を備えて、前記変調波の搬送信号成分
に含まれる複数の前記妨害波を選択的に相殺除去
し得るようにしたことを特徴とする妨害波除去受
信装置。 3 特許請求の範囲第1項または第2項記載の受
信装置において、可変発振周波数の発振手段と、
その発振手段の出力により前記受信した変調波の
搬送信号成分の周波数を順次に変換する周波数変
換手段と、その周波数変換手段の出力から所定狭
帯域の信号成分を抽出する狭帯域波手段と、前
記所定狭帯域の成分を角度復調する角度復調手段
とを備えて、前記受信した変調波の搬送信号成分
から前記妨害波を識別するようにしたことを特徴
とする妨害波除去受信装置。
[Scope of Claims] 1. A carrier wave reproducing means for regenerating a carrier wave component from a carrier signal component of a modulated wave having both sideband transmission components received including an interference wave, and a carrier wave component regenerated by the means at π/2. A carrier phase shifting means for shifting the phase, and synchronization for synchronously detecting the carrier signal component of the received modulated wave in the double-side band transmission band using the recovered carrier component whose phase is shifted by π/2 by the means to extract a quadrature phase component. a detection means, a modulation means for modulating the regenerated and π/2 phase-shifted carrier wave component by the quadrature phase component, and a modulation means for modulating the carrier wave component phase-shifted by regenerating π/2 by the quadrature phase component; at least one that extracts the same frequency component as the wave
and subtraction means for subtracting the extracted same frequency component from the carrier signal component of the received modulated wave to cancel out and remove the interference wave mixed into the double sideband transmission component. An interference wave removal receiving device characterized by: 2. The receiving device according to claim 1, comprising a plurality of said wave means each having a different wave band, and selectively canceling out a plurality of said interference waves included in a carrier signal component of said modulated wave. 1. A receiving device for eliminating interference waves, characterized in that the interference waves can be removed. 3. In the receiving device according to claim 1 or 2, oscillation means with a variable oscillation frequency;
a frequency conversion means for sequentially converting the frequency of the carrier signal component of the received modulated wave by the output of the oscillation means; narrowband wave means for extracting a signal component of a predetermined narrow band from the output of the frequency conversion means; 1. An interference wave removal receiving apparatus, comprising: angle demodulation means for angle demodulating a component of a predetermined narrow band, and identifying the interference wave from a carrier signal component of the received modulated wave.
JP59108620A 1984-05-30 1984-05-30 Disturbance wave eliminating receiver Granted JPS60253325A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59108620A JPS60253325A (en) 1984-05-30 1984-05-30 Disturbance wave eliminating receiver

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59108620A JPS60253325A (en) 1984-05-30 1984-05-30 Disturbance wave eliminating receiver

Publications (2)

Publication Number Publication Date
JPS60253325A JPS60253325A (en) 1985-12-14
JPH0374873B2 true JPH0374873B2 (en) 1991-11-28

Family

ID=14489408

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59108620A Granted JPS60253325A (en) 1984-05-30 1984-05-30 Disturbance wave eliminating receiver

Country Status (1)

Country Link
JP (1) JPS60253325A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3301735B2 (en) 1998-12-08 2002-07-15 日本無線株式会社 Interference wave cancellation device

Also Published As

Publication number Publication date
JPS60253325A (en) 1985-12-14

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